Formation process for lithium-ion batteries

ABSTRACT

A method of charging a battery includes applying a charging voltage to a lithium-ion battery for a period of time after the battery is fully charged. The battery includes a positive electrode having a positive active material, a negative electrode having a negative active material, and an electrolyte. The negative active material includes a lithium titanate material and has a capacity that is less than that of the positive electrode. The charging voltage is greater than a fully charged voltage of the battery, and applying the charging voltage for the period of time is sufficient to cause a zero volt crossing potential of the battery to increase to above a decomposition potential of the positive active material.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a Continuation of U.S. patent application Ser. No. 14/657,759, filed Mar. 13, 2015 (now U.S. Pat. No. 9,899,710), which is a Continuation of U.S. patent application Ser. No. 12/112,979, filed Apr. 30, 2008 (now U.S. Pat. No. 8,980,453), the entire disclosures of which are incorporated by reference herein.

BACKGROUND

The present application relates generally to the field of lithium-ion batteries or cells. More particularly, the present application relates to improved methods for initially charging (i.e., forming) such batteries.

Lithium-ion batteries or cells include one or more positive electrodes, one or more negative electrodes, and an electrolyte provided within a case or housing. Separators made from a porous polymer or other suitable material may also be provided intermediate or between the positive and negative electrodes to prevent direct contact between adjacent electrodes. The positive electrode includes a current collector having an active material provided thereon, and the negative electrode includes a current collector having an active material provided thereon. The active materials for the positive and negative electrodes may be provided on one or both sides of the current collectors.

FIG. 1 shows a schematic representation of a portion of a lithium-ion battery 10 such as that described above. The battery 10 includes a positive electrode 20 that includes a positive current collector 22 and a positive active material 24, a negative electrode 30 that includes a negative current collector 32 and a negative active material 34, an electrolyte material 40, and a separator (e.g., a polymeric microporous separator, not shown) provided intermediate or between the positive electrode 20 and the negative electrode 30. The electrodes 20, 30 may be provided as relatively flat or planar plates or may be wrapped or wound in a spiral or other configuration (e.g., an oval configuration). The electrode may also be provided in a folded configuration.

During charging and discharging of the battery 10, lithium ions move between the positive electrode 20 and the negative electrode 30. For example, when the battery 10 is discharged, lithium ions flow from the negative electrode 30 to the positive electrode 20. In contrast, when the battery 10 is charged, lithium ions flow from the positive electrode 20 to the negative electrode 30.

Once assembly of the battery is complete, an initial charging operation (referred to as a “formation process”) may be performed. During this process, a stable solid-electrolyte-inter-phase (SEI) layer is formed at the negative electrode and also possibly at the positive electrode. These SEI layers act to passivate the electrode-electrolyte interfaces as well as to prevent side-reactions thereafter.

One issue associated with conventional lithium-ion batteries relates to the ability of the batteries to withstand repeated charge cycling that involves discharges to near-zero-volt conditions (so-called “deep discharge” conditions). This deep discharge cycling may decrease the attainable full charge capacity of the batteries, which is known in the art as capacity fade. For example, a battery that initially is charged to 2.8 volts (V) may experience capacity fade with repeated deep discharge cycling such that after 150 cycles the full charge capacity of the battery is much less than the initial capacity.

One consequence of capacity fade in rechargeable batteries is that the batteries will require increasingly frequent charging as the capacity fade progresses. In certain circumstances, this may be relatively inconvenient for the user of the batteries. For example, certain implantable medical devices may utilize rechargeable batteries as a power source. Increasing capacity fade will require the patient to more frequently charge the rechargeable batteries.

Accordingly, it would be advantageous to provide a rechargeable battery (e.g., a lithium-ion battery) with increased resistance to capacity fade for batteries that experience repeated deep discharge cycling.

SUMMARY

An exemplary embodiment relates to a method for producing a battery includes providing a battery having a positive electrode, a negative electrode, and an electrolyte that includes a solvent and a salt. The capacity of the negative electrode is less than that of the positive electrode and the negative electrode includes an active material having an average potential versus a lithium reference electrode of greater than approximately 0.2 volts. The method also includes applying an initial charge to the battery at a voltage that is greater than a fully charged voltage of the battery for a sufficient amount of time to cause at least a portion of the solvent to undergo a reduction reaction. The step of applying an initial charge to the battery acts to increase the irreversible capacity loss of the battery during the initial charge and provides the battery with enhanced tolerance to deep discharge conditions.

Another exemplary embodiment relates to a method for manufacturing a lithium-ion battery that includes providing a battery having a positive electrode, a negative electrode, and an electrolyte. The negative electrode is configured such that the battery is limited by the capacity of the negative electrode and includes an active material having an average potential versus a lithium reference electrode of greater than approximately 0.2 volts. The method also includes charging the battery during a formation process with a voltage that is greater than a fully charged voltage of the battery. During the formation process, the voltage of the negative electrode versus a lithium reference electrode drops to a level where a reduction reaction occurs for at least a portion of the electrolyte. The formation process provides the battery with improved tolerance to overdischarge conditions such that the occurrence of capacity fade with repeated overdischarge cycles is reduced.

Another exemplary embodiment relates to a method for producing a battery that includes applying an initial charge to a lithium-ion battery that comprises an electrolyte, a positive electrode, and a negative electrode. The negative electrode has a lower capacity than the positive electrode and includes a negative active material that has an average potential of greater than approximately 0.2 volts versus a lithium reference electrode. The step of applying an initial charge utilizes a voltage that is greater than a fully charged voltage of the battery and is performed for a sufficient amount of time to form a film at the negative electrode that results from the reduction of the electrolyte. The zero volt crossing potential for the battery is increased to a level greater than the decomposition potential of an active material provided on the positive electrode to provide enhanced tolerance to repeated overdischarge conditions.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross-sectional view of a portion of a lithium-ion battery according to an exemplary embodiment.

FIG. 2 is a schematic cross-sectional view of a portion of a lithium-ion battery according to an exemplary embodiment.

FIG. 3 is a graph illustrating the battery voltage and the voltage of the positive and negative electrodes versus a lithium reference electrode during a battery formation process in which a charging voltage of 2.8 volts is used.

FIG. 4 is a graph illustrating two deep discharge cycles for a battery manufactured using the formation process according to FIG. 3.

FIG. 5 is a graph illustrating the battery voltage and the voltage of the positive and negative electrodes versus a lithium reference electrode during a battery formation process in which a charging voltage of 3.4 volts is used.

FIG. 6 is a graph illustrating two deep discharge cycles for a battery manufactured using the formation process according to FIG. 5.

FIG. 7 is a graph illustrating the resistance to capacity fade for the batteries that were produced using the formation processes according to FIGS. 3 and 5.

FIG. 8 is a schematic view of a system in the form of an implantable medical device implanted within a body or torso of a patient.

FIG. 9 is a schematic view of another system in the form of an implantable medical device.

DETAILED DESCRIPTION

An improved formation process for rechargeable batteries or cells (e.g., lithium-ion batteries) has been developed that allows for the production of batteries having improved resistance to capacity fade, particularly under deep-discharge conditions. The improved formation process utilizes a charging voltage that exceeds the charging voltage utilized in conventional battery formation processes, which in turn acts to produce higher levels of irreversible capacity loss during initial formation. As a result, the zero volt crossing potential for the batteries will be at a higher voltage than would otherwise be possible, which may protect the positive electrode active material from degradation that leads to capacity fade in the battery.

Although the improved formation process may be applicable to batteries having a variety of configurations and chemistries, for simplicity the process will be described with respect to the batteries as described in detail below.

FIG. 2 is a schematic cross-sectional view of a portion of a battery 200 according to an exemplary embodiment that includes at least one positive electrode 210 and at least one negative electrode 220. The size, shape, and configuration of the battery may be selected based on the desired application or other considerations. For example the electrodes may be flat plate electrodes, wound electrodes, or folded electrodes (e.g., Z-fold electrodes). According to other exemplary embodiments, the battery may be a button cell battery, a thin film solid state battery, or another type of lithium-ion battery.

According to an exemplary embodiment, the battery 200 has a rating of between approximately 1 and 1000 milliampere hours (mAh). According to another exemplary embodiment, the battery has a rating of between approximately 100 and 400 mAh. According to another exemplary embodiment, the battery is an approximately 300 mAh battery. According to another exemplary embodiment, the battery is an approximately 75 mAh battery. According to another exemplary embodiment, the battery is an approximately 10 mAh battery.

The battery case or housing (not shown) is formed of a metal or metal alloy such as aluminum or alloys thereof, titanium or alloys thereof, stainless steel, or other suitable materials. According to another exemplary embodiment, the battery case may be made of a plastic material or a plastic-foil laminate material (e.g., an aluminum foil provided intermediate a polyolefin layer and a polyester layer).

An electrolyte is provided intermediate or between the positive and negative electrodes to provide a medium through which lithium ions may travel. The electrolyte may be a liquid (e.g., a lithium salt dissolved in one or more non-aqueous solvents). According to an exemplary embodiment, the electrolyte may be a mixture of ethylene carbonate (EC), ethylmethyl carbonate (EMC) and a 1.0 M salt of LiPF₆. According to another exemplary embodiment, an electrolyte may be used that uses constituents that may commonly be used in lithium batteries (e.g., propylene carbonate, dimethyl carbonate, vinylene carbonate, lithium bis-oxalatoborate salt (sometimes referred to as LiBOB), etc.).

Various other electrolytes may be used according to other exemplary embodiments. According to an exemplary embodiment, the electrolyte may be a lithium salt dissolved in a polymeric material such as poly(ethylene oxide) or silicone. According to another exemplary embodiment, the electrolyte may be an ionic liquid such as N-methyl-N-alkylpyrrolidinium bis(trifluoromethanesulfonyl)imide salts. According to another exemplary embodiment, the electrolyte may be a 3:7 mixture of ethylene carbonate to ethylmethyl carbonate (EC:EMC) in a 1.0 M salt of LiPF₆. According to another exemplary embodiment, the electrolyte may include a polypropylene carbonate solvent and a lithium bis-oxalatoborate salt. According to other exemplary embodiments, the electrolyte may comprise one or more of a PVDF copolymer, a PVDF-polyimide material, and organosilicon polymer, a thermal polymerization gel, a radiation cured acrylate, a particulate with polymer gel, an inorganic gel polymer electrolyte, an inorganic gel-polymer electrolyte, a PVDF gel, polyethylene oxide (PEO), a glass ceramic electrolyte, phosphate glasses, lithium conducting glasses, lithium conducting ceramics, and an inorganic ionic liquid gel, among others.

A separator 250 is provided intermediate or between the positive electrode 210 and the negative electrode 220. According to an exemplary embodiment, the separator 250 is a polymeric material such as a polypropylene/polyethelene copolymer or another polyolefin multilayer laminate that includes micropores formed therein to allow electrolyte and lithium ions to flow from one side of the separator to the other. The thickness of the separator 250 is between approximately 10 micrometers (μm) and 50 μm according to an exemplary embodiment. According to a particular exemplary embodiment, the thickness of the separator is approximately 25 m and the average pore size of the separator is between approximately 0.02 m and 0.1 μm.

The positive electrode 210 includes a current collector 212 made of a conductive material such as a metal. According to an exemplary embodiment, the current collector 212 comprises aluminum or an aluminum alloy.

According to an exemplary embodiment, the thickness of the current collector 212 is between approximately 5 μm and 75 μm. According to a particular exemplary embodiment, the thickness of the current collector 212 is approximately 20 μm. It should also be noted that while the positive current collector 212 has been illustrated and described as being a thin foil material, the positive current collector may have any of a variety of other configurations according to various exemplary embodiments. For example, the positive current collector may be a grid such as a mesh grid, an expanded metal grid, a photochemically etched grid, or the like.

The current collector 212 has a layer of active material 216 provided thereon (e.g., coated on the current collector). While FIG. 3 shows that the active material 216 is provided on only one side of the current collector 212, it should be understood that a layer of active material similar or identical to that shown as active material 216 may be provided or coated on both sides of the current collector 212.

According to an exemplary embodiment, the active material 216 is a material or compound that includes lithium. The lithium included in the active material 216 may be doped and undoped during discharging and charging of the battery, respectively. According to an exemplary embodiment, the active material 216 is lithium cobalt oxide (LiCoO₂). According to other exemplary embodiments, the active material may be provided as one or more additional materials. For example, the active material may be LiMn₂O₄ or a material having the formula LiCo_(x)Ni_((1-x))O₂, where x is between approximately 0.05 and 0.8. According to another exemplary embodiment, the active material is a material of the form LiNi_(x)Co_(y)Mn_((1-x-y))O₂ (e.g., LiNi_(1/3)Co_(1/3)Mn_(1/3)O₂). According to another exemplary embodiment, the active material 216 is a metal-doped variety of one of the aforementioned materials, such as a material of the form LiM_(x)Co_(y)Ni_((1-x-y))O₂, where M is aluminum or titanium and x is between approximately 0.05 and 0.3 and y is between approximately 0.1 and 0.3.

For certain applications, it may be desirable to provide a battery having a cell voltage of greater than approximately 3 volts. In such cases, a higher-voltage active material may be utilized on the positive current collector, such as a material in the form Li_(2-x)Co_(y)Fe_(z)Mn_(4-(x+z))O₈ (e.g., Li₂Co_(0.4)Fe_(0.4)Mn_(3.2)O₈). It is believed that such an active material may charge up to 5.2 volts versus a lithium reference electrode, making it possible to obtain an overall cell voltage of up to approximately 3.7 volts. Other relatively high-voltage active materials that may be used for the positive electrode include LiCoPO₄; LiNiPO₄; Li₂CoPO₄F; Li[Ni_(0.2)Li_(0.2)Mn_(0.6)]O₂; and LiCo_(x)Mn_(2x)O₄ (e.g., LiCo_(0.3)Mn_(1.7)O₄).

According to various other exemplary embodiments, the active material may include a material such as a material of the form Li_(1-x)MO₂ where M is a metal (e.g., LiCoO₂, LiNiO₂, and LiMnO₂), a material of the form Li_(1-W)(M′_(x)M″_(y))O₂ where M′ and M″ are different metals (e.g., Li(Cr_(x)Mn_(1-x))O₂, Li(Al_(x)Mn_(1-x))O₂, Li(Co_(x)M_(1-x))O₂ where M is a metal, Li(Co_(x)Ni_(1-x))O₂, and Li(Co_(x)Fe_(1-x))O₂)), a material of the form Li_(1-w)(Mn_(x)Ni_(y)Co_(z))O₂ (e.g., Li(Mn_(1/3)Ni_(1/3)Co_(1/3))O₂, Li(Mn_(1/3)Ni_(1/3)Co_(1/3-x)Mg_(x))O₂, Li(Mn_(0.4)Ni_(0.4)Co_(0.2))O₂, and Li(Mn_(0.1)Ni_(0.1)C_(0.8))O₂), a material of the form Li_(1-w)(Mn_(x)Ni_(x)Co_(1-2x))O₂, a material of the form Li_(1-w)(Mn_(x)Ni_(y)Co_(z)Al_(w))O₂, a material of the form Li_(1-w)(Ni_(x)Co_(y)Al_(z))O₂ (e.g., Li(Ni_(0.8)Co_(0.15)Al_(0.05))O₂), a material of the form Li_(1-w)(Ni_(x)Co_(y)M_(z))O₂ where M is a metal, a material of the form Li_(1-w)(Ni_(x)Mn_(y)M_(z))O₂ where M is a metal, a material of the form Li(Ni_(x-y)Mn_(y)Cr_(2-x))O₄, LiMn₂O₄, a material of the form LiM′M″₂O₄ where M′ and M″ are different metals (e.g., LiMn_(2-y-z) Ni_(y)O₄, Li_(z)O₄, LiNiCuO₄, LiMn_(1-x)Al_(x)O₄, LiNi_(0.5)Ti_(0.5)O₄, and Li_(1.05)Al_(0.1)Mn_(1.85)O_(4-z)F_(z)), Li₂MnO₃, a material of the form Li_(x)V_(y)O_(z) (e.g., LiV₃O₈, LiV₂O₅, and LiV₆O₁₃), a material of the form LiMPO₄ where M is a metal or LiM_(x)′M″_(1-x)PO₄ where M′ and M″ are different metals (e.g., LiFePO₄, LiFe_(x)M_(1-x)PO₄ where M is a metal, LiVOPO₄, and Li₃V₂(PO₄)₃, and LiMPO_(4x) where M is a metal such as iron or vanadium and X is a halogen such as fluorine, and combinations thereof.

A binder material may also be utilized in conjunction with the layer of active material 216 to bond or hold the various electrode components together. For example, according to an exemplary embodiment, the layer of active material may include a conductive additive such as carbon black and a binder such as polyvinylidine fluoride (PVDF) or an elastomeric polymer.

According to an exemplary embodiment, the thickness of the layer of active material 216 is between approximately 0.1 μm and 3 mm. According to another exemplary embodiment, the thickness of the layer of active material 216 is between approximately 25 μm and 300 μm. According to a particular exemplary embodiment, the thickness of the layer of active material 216 is approximately 75 km.

The negative electrode 220 includes a current collector 222 that is made of a conductive material such as a metal. According to an exemplary embodiment, the current collector 222 is aluminum or an aluminum alloy. One advantageous feature of utilizing an aluminum or aluminum alloy current collector is that such a material is relatively inexpensive and may be relatively easily formed into a current collector. Other advantageous features of using aluminum or an aluminum alloy includes the fact that such materials may have a relatively low density, are relatively highly conductive, are readily weldable, and are generally commercially available. According to another exemplary embodiment, the current collector 222 is titanium or a titanium alloy. According to another exemplary embodiment, the current collector 222 is silver or a silver alloy.

While the negative current collector 222 has been illustrated and described as being a thin foil material, the negative current collector may have any of a variety of other configurations according to various exemplary embodiments. For example, the positive current collector may be a grid such as a mesh grid, an expanded metal grid, a photochemically etched grid, a metallized polymer film, or the like.

According to an exemplary embodiment, the thickness of the current collector 222 is between approximately 100 nm and 100 μm. According to another exemplary embodiment, the thickness of the current collector 222 is between approximately 5 μm and 25 μm. According to a particular exemplary embodiment, the thickness of the current collector 222 is approximately 10 km.

The negative current collector 222 has an active material 224 provided thereon. While FIG. 3 shows that the active material 224 is provided on only one side of the current collector 222, it should be understood that a layer of active material similar or identical to that shown may be provided or coated on both sides of the current collector 222.

According to an exemplary embodiment, the negative active material is selected such that it has an average potential that is greater or equal to approximately 0.2 V versus Li/Li⁺ (e.g., according to one particular exemplary embodiment, the negative active material has an average potential that is greater or equal to approximately 0.3 V versus Li/Li⁺; according to a particularly preferred embodiment, the negative active material is a titanate material having an average potential that is greater or equal to approximately 1.5 V versus Li/Li⁺). The inventors have unexpectedly discovered that the use of negative electrode materials that possess a relatively high average potential versus Li/Li reduces the likelihood of lithium plating. According to one exemplary embodiment, such a negative active material is used in conjunction with a positive active material that has an average potential of greater than approximately 3 V versus Li/Li (e.g., LiCoO₂).

According to an exemplary embodiment, the negative active material 224 is a lithium titanate material such as Li₄Ti₅O₁₂ (sometimes referred to as Li_(1+x)[Li_(1/3)Ti_(5/3)]O₄, with 0≤x<1). Other lithium titanate materials which may be suitable for use as the negative active material may include one or more of the following lithium titanate spinel materials: H_(x)Li_(y-x)TiO_(x)O₄, H_(x)Li_(y-x)TiO_(x)O₄, Li₄M_(x)Ti_(5-x)O₁₂, Li_(x)Ti_(y)O₄, Li_(x)Ti_(y)O₄, Li₄[Ti_(1.67)Li_(0.33-y)M_(y)]O₄, Li₂TiO₃, Li₄Ti_(4.75)V_(0.25)O₁₂, Li₄Ti_(4.75)Fe_(0.25)O_(11.88), Li₄Ti_(4.5)Mn_(0.5)O₁₂, and LiM′M″XO₄ (where M′ is a metal such as nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, niobium, or combinations thereof, M″ is an optional three valent non-transition metal, and X is zirconium, titanium, or a combination of these two). Note that such lithium titanate spinel materials may be used in any state of lithiation (e.g., Li_(4+x)Ti₅O₁₂, where 0≤x≤3).

According to an exemplary embodiment, the lithium titanate may be provided such that at least five percent is in the form of lithium titanate nanoparticles (e.g., having a particle size of less than approximately 500 nanometers). The use of such nonoparticles is intended to provide greater surface area for doping and undoping of lithium ions.

According to other exemplary embodiments, a lithium vanadate (e.g., Li_(1.1)V_(0.9)O₂) material may be used as the negative active material. Other materials having cycling potentials that exceed that of lithium by several hundred millivolts and which may be suitable for use as the negative active material include the materials listed in Table 1. Such materials may be used alone or in combination with the lithium titanates described above and/or any of the other materials listed in Table 1.

TABLE 1 Cycling Potentials (vs Li) Class Compound Vmin Vmax Vavg Oxides TiO₂ (Anatase) 1.4 2 1.80 Oxides WO₂ 0.6 1.3 0.80 Oxides WO₃ 0.5 2.6 1.0  Oxides MoO₂ 1.3 2 1.60 Oxides Nb₂O₅ 1.0 2 1.50 Oxides LiWO₂ 0.75 Oxides Li_(x)MoO₂ 0.8 2 1.60 Oxides V₆O₁₃ 2.30 Oxides Li₆Fe₂O₃ 0.75 Oxides LiFeO₂ 1.0 3.0 2.0  Oxides Fe₂O₃ 0.2 2.0 0.75 Oxides MO where M = Co, Ni, Cu or Fe 0.8-1.5 Sulfides FeS₂ 1.3 1.9 1.65 Sulfides MoS₂ 1.75 Sulfides TiS₂ 2.00 Alloys Sn—Bi 0.75 Alloys Alloys comprising of Al, Si or Sn 0.30 and other elements Alloys Sn—Co—C 0.30 Alloys Sb 0.90 Alloys NbSe₃ 1.95 Alloys Bi 0.80 Alloys In 0.60 Alloys LixAl 0.36 Alloys LixSn 0 1.3 0.50 Alloys Sn—Sb 0.0-1.0 Polymers Poly(phenylquinoline) 1.50 Polymers Polyparaphenylene 0.70 Polymers Polyacetylene 1.00 Vanadates Li_(x)MVO₄ where M = Ni, Co, Cd, 2.0-0.5 Zn

A binder material may also be utilized in conjunction with the layer of active material 224. For example, according to an exemplary embodiment, the layer of active material may include a binder such as polyvinylidine fluoride (PVDF) or an elastomeric polymer. The active material 224 may also include a conductive material such as carbon (e.g., carbon black) at weight loadings of between zero and ten percent to provide increased electronic conductivity.

According to various exemplary embodiments, the thickness of the active material 224 is between approximately 0.1 μm and 3 mm. According to other exemplary embodiments, the thickness of the active material 224 may be between approximately 25 μm and 300 μm. According to another exemplary embodiment, the thickness of the active material 224 may be between approximately 20 μm and 90 μm, and according to a particular exemplary embodiment, approximately 75 μm.

Lithium plating occurs when the potential of the negative electrode versus a lithium reference electrode reaches 0 volts, and is a well-known phenomenon that can lead to loss in performance of lithium-ion batteries. When used in a negative electrode of a lithium-ion battery, lithium titanate active materials cycle lithium at a potential plateau of about 1.55 volts (which is substantially higher than graphitic carbon, which cycles lithium at approximately 0.1 volts in the fully charged state). As a result, batteries using lithium titanate as a negative active material are less susceptible to lithium plating than those using carbon-based materials for the negative active material.

One potential advantageous feature of utilizing a negative electrode active material such as a lithium titanate material or another material having an average potential that is greater or equal to approximately 0.2 V versus Li/Li⁺ is that more favorable design rules may be possible. One such design rule relates to the cell balance parameters.

Cell balance refers to the ratio of the negative electrode capacity to the positive electrode capacity. Thus, the cell balance γ (gamma) can thus be expressed as an equation having the form:

$\gamma = \frac{Q_{neg}}{Q_{pos}}$

where Q_(neg) is equal to the product of the amount of negative electrode material, the percentage of the active material contributing to the capacity, and the specific capacity of the active material and Q_(pos) is equal to the product of the amount of positive material, the percent of the active material contributing to the capacity, and the specific capacity of active material. According to an exemplary embodiment in which a lithium titanate negative active material and a lithium cobalt oxide positive active material are used, the specific capacity of the negative active material may be 165 mAh/g (at C/3-C/1, between 1.2 and 2.0 volts versus Li) and the specific capacity of the positive active material may be 150 mAh/g (at C/3-C/1, between 4.25 and 3.0 volts versus Li).

Cell balance dictates the mass (deposition) ratio of the two electrodes. In conjunction with charge cutoff voltage, cell balance determines what fraction of the active Li sites in the two electrode materials is utilized during charge and discharge. For example, in a negative-limited design, nearly all active Li sites in the negative material are utilized in the negative electrode, but only a fraction of the active sites in the positive electrode are utilized, and vice versa. The chosen cell balance hence determines the specific capacity delivered by both electrodes, and the stability of their performance for repeated cycling. Primary considerations for choosing the cell balance include safety, delivered capacity and capacity fade under regular cycling and deep discharge conditions.

Lithium-ion batteries using carbon-based negative active materials are typically fabricated such that the capacity of the electrodes is balanced (i.e., the capacities of the positive electrode and negative electrode are equal) or positive-limited (i.e., the capacity of the positive electrode is less than that of the negative electrode). The reason for this design rule is that if the battery was negative-limited, the voltage of the negative electrode versus a lithium reference electrode would drop to near zero volts during charging of the battery, which may result in lithium plating (since carbonaceous negative electrodes typically operate very close to potential of metallic Li (0.1-0.2 volts versus Li), and a further decrease in potential at the negative electrode would result in plating of lithium).

According to an exemplary embodiment in which a battery utilizes a negative electrode active material such as a lithium titanate material or another material having an average potential that is greater or equal to approximately 0.2 volts versus a lithium reference electrode, the battery may be fabricated with a negative-limited design in which the capacity of the negative electrode is less than that of the positive electrode. For example, for a lithium titanate active material having a potential plateau of approximately 1.55 volts, a cell balance of between approximately 0.80 to 0.90 may be used (i.e., the nominal capacity of the negative electrode may be between 80 and 90 percent of the nominal capacity of the positive electrode). According to another exemplary embodiment, the cell balance may be less than approximately 0.8 (e.g., 0.78).

Batteries such as those described herein having a negative-limited design may provide a number of advantages. For example, when charged using the formation process described below, such batteries may exhibit lower capacity fade and lower power fade due to reduced likelihood of over-charging of the positive electrode. Other advantages include the ability to more rapidly recharge the battery without risking polarization of the positive electrode to high potentials, which also helps reduce capacity fade. Further, with a negative limited design, additives which prevent degradation due to oxidation of the positive electrode are not required. This not only reduces cost, but also makes the electrolyte chemistry simpler. Such additives typically lead to gas formation and swelling when oxidized, and all of that is eliminated in the negative limited design. Another advantage of a negative limited design over a positive limited design, which may depend in part on the specific choice of materials used, is that negative limited design offers higher energy density. For example, a lithium titanate material used for a negative has a lower density than a lithium cobalt oxide positive active material—with a negative limited cell design, the proportion of the negative material required is less, which offers better volumetric efficiency.

One particular advantage associated with negative-limited batteries (using negative active materials such as a lithium titanate material or another material having an average potential that is greater or equal to approximately 0.2 volts versus a lithium reference electrode) is described with respect to FIGS. 3-7. According to an exemplary embodiment, an improved formation process may be used in conjunction with such batteries that provides enhanced tolerance to repeated deep discharge conditions, as evidenced, for example, by improved resistance to capacity fade.

During a formation (i.e., initial charging of the battery) process, lithium-ion batteries are charged at a relatively low rate (such as C/10 or slower) to the maximum operating voltage of the battery. By way of example, for a lithium-ion battery (LiCoO₂ positive active material, lithium titanate negative active material) that is configured to have an intended operating voltage range between approximately 2.8 volts (full charge) and 1.8 volts (discharge cut-off voltage), a formation process might involve charging the battery at a voltage of 2.8 volts at a rate of C/10 and then holding the battery at the 2.8 volt level for four hours. FIG. 3 illustrates the voltage behavior for a battery undergoing such a formation process, and includes a curve 310 representative of the overall battery voltage, a curve 312 representative of the positive electrode potential versus a lithium reference electrode, and a curve 314 representative of the negative electrode potential versus a lithium reference electrode. As shown in FIG. 3, the overall battery voltage gradually increases to a 2.8 volt plateau 311 at the end of formation process, while the negative electrode potential versus a lithium reference electrode drops to a level of between approximately 1.3 and 1.4 volts toward the end of curve 314.

The formation process described in the preceding paragraph may result in a relatively low irreversible capacity loss for the battery (e.g., between approximately 6 and 11 percent) during the formation process. This irreversible capacity loss results primarily from the passivation of the two electrodes, and occurs when otherwise cyclable lithium ions in the battery (i.e., lithium ions that shuttle between the positive and negative electrodes during charging and discharging) combine with an electrode active material.

FIG. 4 illustrates the voltage behavior for the battery when it is subjected to two deep discharge cycles where the battery is discharged to zero volts, and includes a curve 320 representative of the overall battery voltage, a curve 322 representative of the positive electrode potential versus a lithium reference electrode, and a curve 324 representative of the negative electrode potential versus a lithium reference electrode. As the overall battery voltage drops toward zero volts (i.e., a deep discharge condition), the curves 322, 324 representing the potentials of the positive and negative electrodes converge toward and intersect at a point 326 referred to as the zero volt crossing potential for the battery. As illustrated in FIG. 4, the zero voltage crossing potential for this battery occurs at a point where the positive electrode potential versus a lithium reference electrode is less than 2.0 volts (e.g., between approximately 1.6 and 1.8 volts).

FIG. 7 is a graph that includes a curve 330 representative of the discharge capacity of the battery as it undergoes repeated deep discharge cycles. The variations in the curves at cycles 50 and 100 are a result of two characterization cycles that were run during the test. These characterization cycles consist of (1) a slow rate cycle to determine trends in full charge/discharge capacity, (2) an application rate cycle to determine impact of repeated deep discharge on performance in normal application conditions. Other smaller variations (such as around cycle 170) are experimental artifacts.

As illustrated by the curve 330 shown in FIG. 7, the discharge capacity of the battery drops as it is subjected to repeated deep discharge cycles. This capacity fade with repeated deep discharge cycles results in a battery that must be recharged more frequently, since the battery does not hold as much charge as it did after initial formation.

The inventors have determined through experimentation that one factor that contributes to the capacity fade is that the positive active material (in this case LiCoO₂) tends to relatively rapidly degrade when driven to a potential versus a lithium reference electrode that is less than 2.0 volts (e.g., approximately 1.6 volts). It should be noted that where different positive active materials are used, degradation of such materials may occur at a different level. As illustrated in FIG. 4, the potential of the positive electrode versus a lithium reference electrode, as represented by curve 322, drops to a level that is below 2.0 volts as the battery is discharged to a near-zero-volt charge state and the curves 322, 324 approach the zero volt crossing potential 326 for the battery.

The inventors have surprisingly discovered that the resistance to capacity fade for a negative-limited battery that utilizes a lithium titanate active material on the negative electrode can be significantly improved by using a formation process in which the charging voltage is greater than the normal fully charged voltage of the battery, with no associated increase in charging rate (e.g., the same C/10 charging rate may be used as described in the preceding example).

According to an exemplary embodiment, a lithium-ion battery (LiCoO₂ positive active material, lithium titanate negative active material) having an intended operating voltage range from 2.8 volts (fully charged state) to 1.8 volts (cut-off voltage) is subjected to a formation process that utilizes a charging voltage of between approximately 3.4 volts and 3.8 volts at a C/10 charge rate, after which the battery voltage is held at this level for a period of between approximately 4 and 12 hours. FIG. 5 illustrates the voltage behavior for a battery undergoing such a formation process, and includes a curve 340 representative of the overall battery voltage, a curve 342 representative of the positive electrode potential versus a lithium reference electrode, and a curve 344 representative of the negative electrode potential versus a lithium reference electrode.

As shown in FIG. 5, the battery voltage gradually increases to a 3.4 volt plateau 341 at the end of formation process. The higher charging voltage during the formation process results in a greater amount of irreversible capacity loss as compared to formation process using a lower charging voltage (e.g., 2.8 volts). For example, the total irreversible capacity loss obtained using the higher-voltage formation process is expected to be between approximately 12 and 20 percent, depending on factors including, for example, the selected cut-off voltage and hold duration.

The negative electrode potential versus a lithium reference electrode drops to a level below approximately 0.9 volts (e.g., between approximately 0.5 and 0.8 volts) as the battery reaches its fully charged state (i.e., the charge top-off voltage during normal use), while the positive electrode potential does not exhibit a large voltage increase. This is primarily due to the fact that the battery is negative-limited such that the capacity of the negative electrode is less than that of the positive electrode (i.e., the negative electrode depletes before the positive electrode, which results in a potential drop for the negative electrode).

As the potential of the negative electrode drops below approximately 0.9 volts, a reaction takes place in which the solvent component of the electrolyte (e.g., ethylene carbonate) reduces. In this reduction reaction, a passive film (e.g., lithium carbonate or lithium alkyl carbonate) is formed on the negative electrode. Additionally, an additive such as carbon or a carbon-based material may be provided in the negative active material to assist in the formation of the passive film and to increase the amount of lithium that reacts irreversibly to form the film (e.g., between approximately 5 and 10 volume percent carbon may be provided in the lithium titanate material).

One advantageous feature of the reduction reaction is that the increased irreversible capacity loss of the battery tends to increase the zero volt crossing potential for the battery, which allows for enhanced resistance to capacity fade since the higher zero volt crossing potential is above the level where the positive active material degrades.

FIG. 6 illustrates the voltage behavior for such a battery when it is subjected to two deep discharge cycles where the battery is discharged to zero volts, and includes a curve 350 representative of the overall battery voltage, a curve 352 representative of the positive electrode potential versus a lithium reference electrode, and a curve 354 representative of the negative electrode potential versus a lithium reference electrode. As the overall battery voltage drops toward zero volts (i.e., a deep discharge condition), the curves 352, 354 representing the potentials of the positive and negative electrodes converge toward and intersect at the zero volt crossing potential 356 for the battery. As illustrated in FIG. 6, the zero voltage crossing potential for this battery occurs at a point where the positive electrode potential versus a lithium reference electrode is greater than approximately 3.5 volts, which is above the threshold at which the positive active material (LiCoO₂) would be expected to degrade. It should also be noted that the lithium titanate negative electrode active material is also stable at this potential.

The battery produced using the high-voltage formation process exhibits significantly enhanced resistance to capacity fade when subjected to repeated deep discharge cycles, as illustrated by the curve 360 in FIG. 7. The capacity of the battery is substantially constant over approximately 170 deep discharge cycles, in contrast to the relatively significant capacity fade exhibited by the battery using a more conventional formation process (curve 330).

Accordingly, the use of a voltage that exceeds the voltage of the fully charged battery during the formation process acts to induce a larger amount of irreversible capacity loss in the battery than would otherwise be obtained. This in turn increases the zero voltage crossing potential for the battery above the level where the positive active material would degrade. As a result, the resistance to capacity fade with repeated deep discharge cycles is enhanced.

Example 1

Lithium ion cells having nominal capacities of approximately 0.15 ampere hours (Ah) were prepared having a lithium cobalt oxide (LiCoO₂) active material on the positive electrode and a lithium titanate active material on the negative electrode. The electrolyte used included a mixture of ethylene carbonate, ethylmethyl carbonate, and 1 molar LiPF₆ as the lithium salt. The cells were constructed as spirally wound prismatic cells hermetically sealed in a stainless steel can with a glass feedthrough.

The negative and positive electrodes for the cells were prepared via a slurry coating and calendaring process. Both electrodes included the aforementioned active material, a conductive carbon additive, and organic binder. The mass loading (grams of materials per unit area) during the slurry coating process was controlled on both electrodes to attain a mass ratio of the two active materials to be 0.71. Based on the nominal specific capacities of the two active materials, determined via half cell testing (150 mAh/g for lithium cobalt oxide, 165 mAh/g for lithium titanate), the cell balance of this cell was 0.78 (i.e., the nominal capacity of the negative electrode was 78% of the nominal capacity of the positive electrode).

Cells built with the above design were subjected to a conventional formation process in which the cells were charged at C/10 (15 mA) to the normal cut-off voltage of 2.8 volts and were held potentiostatically at 2.8 volts for 4 hours. Another group of cells built with the above design were subjected to an improved high voltage formation process. In this process, the cells were charged at C/10 (15 mA) to 3.4 volts and were held potentiostatically at 3.4 volts for 4 hours. After these respective formation processes, both groups of cells were discharged at C/10 to 1.8 volts and held at 1.8 volts for 4 hours.

The capacities delivered by the cells were measured both during the formation charge process and during the discharge process. The measured capacity values are given in Table 2. The formation charge capacity is typically greater than the discharge capacity, which is indicative of the irreversible capacity loss accounted for by the irreversible processes. The cells show 6.5% irreversible capacity during the conventional formation process, compared to 12.2% in the improved high voltage formation process. Thus, the difference in the irreversible capacities is approximately 5.7% between the 2.8 volts formation and high voltage 3.4 volts formation. This difference is seen to increase as a greater voltage and/or a longer potentiostatic hold duration is chosen. It is noteworthy that this greater irreversible capacity does not reduce the reversible capacity of the cell. Cycle 1 discharge capacity is the same for both groups of cells, as shown in Table 2. The higher irreversible capacity is attained by extending the voltage window beyond its normal cut-off and thus comes out from the extended capacity and not from the nominal capacity over the voltage range for normal cycling. Thus, unlike typical cases where higher irreversible capacity means lower irreversible capacity, such a lowering of the reversible capacity was not observed.

TABLE 2 Cycle 1 Cycle 1 Cycle 160 % Fade charge discharge Cycle 160 discharge between capacity Capacity charge capacity cycles 1 (Ah) (Ah) capacity (Ah) (Ah) and 160 Cells 0.168 0.157 0.081 0.081 48.4% formed at 2.8 volts Cells 0.180 0.158 0.152 0.152 3.5% formed at 3.4 volts

These cells were then cycled between 2.8 volts to 0.0 volts to determine the stability of performance for repeated deep discharge to zero volts. During the charge phase of this cycling, the cells were taken to 2.8 volts at a 1C rate (150 mA) and potentiostatically held at 2.8 volts for 1 hour. During the discharge phase of the cycling, the cells were taken to 0.0 volts in a staged manner—first the cells were discharged to 1.8 volts at 150 mA, held potentiostatically at 1.8 volts for 1 hour, then discharged to 0.0 volts at 0.1 mA and finally held potentiostatically at 0.0 volts for 24 hours. The difference in performance of the two groups of cells in this test is shown in FIG. 7, where the capacity obtained in every cycle as a percent of the initial capacity is plotted versus the cycle number. The cells with the conventional formation show large capacity fade, with the capacity falling to approximately 52% after 160 deep discharge cycles. In sharp contrast, the cells with the high voltage formation continue to show greater than 95% of the initial capacity after 160 deep discharge cycles.

The batteries and formation methods described in the preceding Example 1 and elsewhere in the present application may find utility in a variety of applications, including in implantable medical devices (IMDs). FIG. 8 illustrates a schematic view of a system 400 (e.g., an implantable medical device) implanted within a body or torso 432 of a patient 430. The system 400 includes a device 410 in the form of an implantable medical device that for purposes of illustration is shown as a defibrillator configured to provide a therapeutic high voltage (e.g., 700 volt) treatment for the patient 430.

The device 410 includes a container or housing 414 that is hermetically sealed and biologically inert according to an exemplary embodiment. The container may be made of a conductive material. One or more leads 416 electrically connect the device 410 and to the patient's heart 420 via a vein 422. Electrodes 417 are provided to sense cardiac activity and/or provide an electrical potential to the heart 420. At least a portion of the leads 416 (e.g., an end portion of the leads shown as exposed electrodes 417) may be provided adjacent or in contact with one or more of a ventricle and an atrium of the heart 420.

The device 410 includes a battery 440 provided therein to provide power for the device 410. The size and capacity of the battery 440 may be chosen based on a number of factors, including the amount of charge required for a given patient's physical or medical characteristics, the size or configuration of the device, and any of a variety of other factors. According to an exemplary embodiment, the battery is a 5 mAh battery. According to another exemplary embodiment, the battery is a 300 mAh battery. According to various other exemplary embodiments, the battery may have a capacity of between approximately 1 and 1000 mAh.

According to other exemplary embodiments, more than one battery may be provided to power the device 410. In such exemplary embodiments, the batteries may have the same capacity or one or more of the batteries may have a higher or lower capacity than the other battery or batteries. For example, according to an exemplary embodiment, one of the batteries may have a capacity of approximately 500 mAh while another of the batteries may have a capacity of approximately 75 mAh.

According to an exemplary embodiment, the battery may be configured such that it may be charged and recharged using an inductive charging system in which a primary or external coil is provided at an exterior surface of a portion of the body (either proximate or some distance away from the battery) and a secondary or internal coil is provided below the skin adjacent the primary coil.

According to another exemplary embodiment shown in FIG. 9, an implantable neurological stimulation device 500 (an implantable neuro stimulator or INS) may include a battery 502 such as those described above with respect to the various exemplary embodiments. Examples of some neuro stimulation products and related components are shown and described in a brochure titled “Implantable Neurostimulation Systems” available from Medtronic, Inc.

An INS generates one or more electrical stimulation signals that are used to influence the human nervous system or organs. Electrical contacts carried on the distal end of a lead are placed at the desired stimulation site such as the spine or brain and the proximal end of the lead is connected to the INS. The INS is then surgically implanted into an individual such as into a subcutaneous pocket in the abdomen, pectoral region, or upper buttocks area. A clinician programs the INS with a therapy using a programmer. The therapy configures parameters of the stimulation signal for the specific patient's therapy. An INS can be used to treat conditions such as pain, incontinence, movement disorders such as epilepsy and Parkinson's disease, and sleep apnea. Additional therapies appear promising to treat a variety of physiological, psychological, and emotional conditions. Before an INS is implanted to deliver a therapy, an external screener that replicates some or all of the INS functions is typically connected to the patient to evaluate the efficacy of the proposed therapy.

The INS 500 includes a lead extension 522 and a stimulation lead 524. The stimulation lead 524 is one or more insulated electrical conductors with a connector 532 on the proximal end and electrical contacts (not shown) on the distal end. Some stimulation leads are designed to be inserted into a patient percutaneously, such as the Model 3487A Pisces-Quad® lead available from Medtronic, Inc. of Minneapolis Minn., and stimulation some leads are designed to be surgically implanted, such as the Model 3998 Specify® lead also available from Medtronic.

Although the lead connector 532 can be connected directly to the INS 500 (e.g., at a point 536), typically the lead connector 532 is connected to a lead extension 522. The lead extension 522, such as a Model 7495 available from Medtronic, is then connected to the INS 500.

Implantation of an INS 500 typically begins with implantation of at least one stimulation lead 524, usually while the patient is under a local anesthetic. The stimulation lead 524 can either be percutaneously or surgically implanted. Once the stimulation lead 524 has been implanted and positioned, the stimulation lead's 524 distal end is typically anchored into position to minimize movement of the stimulation lead 524 after implantation. The stimulation lead's 524 proximal end can be configured to connect to a lead extension 522.

The INS 500 is programmed with a therapy and the therapy is often modified to optimize the therapy for the patient (i.e., the INS may be programmed with a plurality of programs or therapies such that an appropriate therapy may be administered in a given situation).

A physician programmer and a patient programmer (not shown) may also be provided to allow a physician or a patient to control the administration of various therapies. A physician programmer, also known as a console programmer, uses telemetry to communicate with the implanted INS 500, so a clinician can program and manage a patient's therapy stored in the INS 500, troubleshoot the patient's INS system, and/or collect data. An example of a physician programmer is a Model 7432 Console Programmer available from Medtronic. A patient programmer also uses telemetry to communicate with the INS 500, so the patient can manage some aspects of her therapy as defined by the clinician. An example of a patient programmer is a Model 7434 Itrel® 3 EZ Patient Programmer available from Medtronic.

According to an exemplary embodiment, a battery provided as part of the INS 500 may be configured such that it may be charged and recharged using an inductive charging system in which a primary or external coil is provided at an exterior surface of a portion of the body (either proximate or some distance away from the battery) and a secondary or internal coil is provided below the skin adjacent the primary coil.

While the medical devices described herein (e.g., systems 400 and 500) are shown and described as a defibrillator and a neurological stimulation device, it should be appreciated that other types of implantable medical devices may be utilized according to other exemplary embodiments, such as pacemakers, cardioverters, cardiac contractility modules, drug administering devices, diagnostic recorders, cochlear implants, and the like for alleviating the adverse effects of various health ailments.

It is also contemplated that the medical devices described herein may be charged or recharged when the medical device is implanted within a patient. That is, according to an exemplary embodiment, there is no need to disconnect or remove the medical device from the patient in order to charge or recharge the medical device.

It is important to note that the construction and arrangement of the batteries and cells and the methods for forming such batteries as shown and described in the various exemplary embodiments is illustrative only. Although only a few embodiments have been described in detail in this disclosure, those skilled in the art who review this disclosure will readily appreciate that many modifications are possible without materially departing from the novel teachings and advantages of the subject matter recited in the claims. Accordingly, all such modifications are intended to be included within the scope of the present invention as defined in the appended claims. The order or sequence of any process or method steps may be varied or re-sequenced according to other exemplary embodiments. Other substitutions, modifications, changes, and omissions may be made in the design, operating conditions, and arrangement of the various exemplary embodiments without departing from the scope of the present inventions as expressed in the appended claims. 

1-20. (canceled)
 21. A method of charging a battery comprising: applying a charging voltage to a lithium-ion battery for a period of time after the battery is fully charged, the battery comprising a positive electrode having a positive active material, a negative electrode having a negative active material comprising a lithium titanate material and having a capacity that is less than that of the positive electrode, and an electrolyte; wherein the charging voltage is greater than a fully charged voltage of the battery, and applying the charging voltage for the period of time is sufficient to cause a zero volt crossing potential of the battery to increase to above a decomposition potential of the positive active material.
 22. The method according to claim 21, wherein the lithium titanate material is selected from the group consisting of Li₂TiO₃, Li₄Ti_(4.75)V_(0.25)O₁₂, Li₄Ti_(4.75)Fe_(0.25)O_(11.88), Li₄Ti_(4.5)Mn_(0.5)O₁₂, and combinations thereof.
 23. The method according to claim 21, wherein the lithium titanate material is selected from the group consisting of H_(x)Li_(y-x)TiO_(x)O₄, H_(x)Li_(y-x)TiO_(x)O₄, Li₄M_(x)Ti_(5-x)O₁₂, Li_(x)Ti_(y)O₄, Li_(x)Ti_(y)O₄, Li₄[Ti_(1.67)Li_(0.33-y)M_(y)]O₄, and combinations thereof.
 24. The method according to claim 23, wherein x is between approximately 0 and
 3. 25. The method according to claim 21, wherein the lithium titanate material comprises LiM′XO₄, wherein M′ is a metal comprising nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium, and X comprises zirconium or titanium.
 26. The method according to claim 25, wherein M′ comprises a combination of at least two of nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium.
 27. The method according to claim 25, wherein X comprises a combination of zirconium and titanium.
 28. The method according to claim 21, wherein the lithium titanate material comprises LiM′M″XO₄, wherein M′ is a metal comprising nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium, M″ is a three valent non-transition metal, and X comprises zirconium or titanium.
 29. The method according to claim 28, wherein M′ comprises a combination of at least two of nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium.
 30. The method according to claim 28, wherein X comprises a combination of zirconium and titanium.
 31. A method of charging a battery comprising: providing a lithium-ion battery comprising a positive electrode having a positive active material, a negative electrode having a negative active material comprising a lithium titanate material and having a capacity that is less than that of the positive electrode, and an electrolyte having a solvent, wherein the negative active material has an average cycling potential versus a lithium reference electrode that is greater than a reduction potential at or below which the solvent reduces; and applying a charging voltage to the battery for a duration while the battery is fully charged, wherein the charging voltage and the duration are sufficient to cause a potential of the negative electrode to fall below the reduction potential.
 32. The method according to claim 31, wherein the lithium titanate material is selected from the group consisting of Li₂TiO₃, Li₄Ti_(4.75)V_(0.25)O₁₂, Li₄Ti_(4.75)Fe_(0.25)O_(11.88), Li₄Ti_(4.5)Mn_(0.5)O₁₂, and combinations thereof.
 33. The method according to claim 31, wherein the lithium titanate material is selected from the group consisting of H_(x)Li_(y-x)TiO_(x)O₄, H_(x)Li_(y-x)TiO_(x)O₄, Li₄M_(x)Ti_(5-x)O₁₂, Li_(x)Ti_(y)O₄, Li_(x)Ti_(y)O₄, Li₄[Ti_(1.67)Li_(0.33-y)M_(y)]O₄, and combinations thereof.
 34. The method according to claim 33, wherein x is between approximately 0 and
 3. 35. The method according to claim 31, wherein the lithium titanate comprises LiM′XO₄, wherein M′ is a metal comprising nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium, and X comprises zirconium or titanium.
 36. The method according to claim 35, wherein M′ comprises a combination of at least two of nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium.
 37. The method according to claim 35, wherein X comprises a combination of zirconium and titanium.
 38. The method according to claim 31, wherein the lithium titanate comprises LiM′M″XO₄, wherein M′ is a metal comprising nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium, M″ is a three valent non-transition metal, and X comprises zirconium or titanium.
 39. The method according to claim 38, wherein M′ comprises a combination of at least two of nickel, cobalt, iron, manganese, vanadium, copper, chromium, molybdenum, or niobium.
 40. The method according to claim 38, wherein X comprises a combination of zirconium and titanium. 